One can try to interpret the lattice theory as a manifestly diffeomorphism-invariant construction, with
the lattice representing an entire diffeomorphism equivalence class of lattices embedded in the
continuum [146]. In order to make this interpretation consistent, one should modify the functional form of
either the Hamiltonian or the measure, in such a way that the commutator of two lattice Hamiltonians
vanishes, as
.
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